Differential Color Sensor Without Filters

ABSTRACT

A semiconductor color sensor implemented without the use of color filters. Fabricating photodiodes using different semiconductor materials provide photodiodes with different sensitivities vs. wavelengths. A first embodiment uses photodiodes with different junction depths. A shallow junction depth produces a photodiode with its sensitivity peak in shorter wavelengths, while a deeper junction depth produces a photodiode with its sensitivity peak in longer wavelengths. Amorphous as well as crystalline structures may be used. A second embodiment uses photodiodes with different materials, such as Silicon-Germanium (SiGe) which has a longer wavelength peak sensitivity, and Silicon (Si) which has a shorter wavelength peak sensitivity in comparison. More than two photodiodes having different wavelength sensitivities may be used. Sensing current ratios between pairs of diodes allows color balance to be maintained.

TECHNICAL FIELD

Embodiments in accordance with the invention are related to solid-state color sensors.

BACKGROUND

Sensing the spectral content of incident light is important in many arenas, for example in determining and/or maintaining color balance in displays comprised of light emitting diode (LED) displays of different colors.

One approach to such sensing as known to the art involves a plurality of photodiodes combined with filters which selectively pass light of predetermined wavelengths. The performance of such sensors is limited by the accuracy of the light transmission characteristics of the filters, and the long-term performance is limited by the long-term stability of the filters. Sensitivity is also impacted by filters, as they are typically absorptive. Furthermore the selectivity of such color sensors is usually limited by the availability of filtering materials.

SUMMARY OF THE INVENTION

A first photodiode sensor with a sensitivity peak in the shorter wavelengths and a second photodiode sensor with a sensitivity peak in the longer wavelengths are used to monitor the spectral content of incident light. Shifts in spectra content will cause the ratio of photocurrents between the first and second sensors to change. Measuring the ratio is preferred to absolute measurements.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows absorption depth vs. wavelength for Silicon (Si) and Silicon-Germanium (SiGe),

FIG. 2 shows ratio determination by analog means, and

FIG. 3 shows ratio determination by digital means.

DETAILED DESCRIPTION OF THE EMBODIMENTS

Germanium

According to the present invention, a differential color sensor uses a first photodiode sensor with a sensitivity peak in shorter wavelengths and a second photodiode sensor with a sensitivity peak in longer wavelengths to monitor the spectral content of incident light.

In a first embodiment of the invention, different semiconductor materials are used. A first embodiment uses a Silicon (Si) photodiode, which has its sensitivity peak in shorter wavelengths, and a Silicon-Germanium (SiGe) photodiode, which has its sensitivity peak in the longer wavelengths.

In a second embodiment of the invention, photodiodes with different junction depths are used. A photodiode with a shallow junction depth has its sensitivity peak in shorter wavelengths, and a photodiode with a deeper junction depth has its sensitivity peak in longer wavelengths.

These differences are shown in FIG. 1, which shows Silicon photo absorption depths with respect to wavelengths. Curve 100 shows absorption depths for Silicon, with red, green, and blue indicate. Curve 110 shows absorption depths for Silicon-Germanium (SiGe, 20% Ge). This shows that color sensors with differing junction depths, for example, 0.2 um, 0.8 um, and 3.0 um in Silicon can provide good color sensors, and the response difference between Silicon and Silicone-Germanium photodiodes.

In a third embodiment of the invention, or in combination with previously disclosed embodiments, amorphous material may be used in photodiodes, as well as more common crystalline structures.

Using a pair of photodiodes as a color sensor, two separately packaged diodes may be used. Integration may be furthered by packaging two distinct diodes in one optical package, and improved further by fabricating both diodes on the same die.

In a first embodiment, photodiodes with different sensitivities vs. wavelengths may be implemented without the use of color filters by fabricating photodiodes using different semiconductor materials. Semiconductor materials with differing bandgap voltages will have different sensitivity vs. wavelength properties, such as the difference between pure Silicon (Si), and Silicon-Germanium (SiGe). As an example, using two diodes each with a junction depth of 0.5 um in Silicon and Silicon-Germanium will produce different spectral peak responses, as evident from FIG. 1.

In a second embodiment, photodiodes with different sensitivities vs. wavelengths may be implemented by altering the photodiode junction depth. A shallow junction depth produces a photodiode with its sensitivity peak in shorter wavelengths, while a deeper junction depth produces a photodiode with its sensitivity peak in longer wavelengths.

Amorphous materials may also be used, as a third embodiment or in combination with other embodiments. As an example, amorphous photodiodes may be used with differing junction depths. Amorphous diodes such as amorphous Silicon and amorphous Silicon-Germanium may be used.

In application, as shown in FIG. 2, photodiode 100 drives transimpedance amplifier 110, which has its gain set by feedback resistor 120. This transimpedance amplifier converts photocurrent from photodiode 100 to a voltage output 130. With a feedback resistor 120 of 1 megOhm, this output is 1 volt per microAmp of photodiode current. Similarly, photodiode 150 drives transimpedance amplifier 160, with feedback set by resistor 170, producing voltage output 180. These two voltages feed ratio circuit 200, producing a voltage ratio at output 210. Various ratio circuits may be used, as will be apparent to one skilled in the art. One such ratio circuit is shown on page 31 of Application Note 31 Op Amp Circuit Collection, published by National Semiconductor Corporation, September 2002. Four-quadrant analog multipliers, such as the AD633 from Analog Devices may also be used. Similarly, other current to voltage converters may be used with photodiodes 100 and 150, such as shown on page 3 of the aforementioned Application Note 31 Op Amp Circuit Collection. The sum of the photocurrents which may be calculated as a weighted sum, may be used as an indication of intensity.

As shown in FIG. 37 the ratio of the two photocurrents may also be produced in digital fashion. Photodiodes 110 and 150 drive transimpedance amplifiers 110 and 160 as in FIG. 3, producing voltage outputs for the two photodiodes. These voltages are fed to analog to digital converter (ADC) 200, which converts the analog voltages to digital form. Suitable ADCs are made by companies such as Linear Technologies. Multiple single-channel ADCs, an analog multiplexer feeding a single-channel ADC, or a multiple-channel ADC may be used. A custom analog to digital converter could integrate the transimpedance amplifiers, or eliminate them entirely. The digital values of the input voltages are then handled by a microprocessor, not shown, to derive the ratio.

By using either an analog or a digital control loop to hold the ratio constant while driving a plurality of different color emitters such as light emitting diodes or laser diodes, color may be held constant. Digital schemes such as the well-known PD controller (Proportional, Integral, Derivative) may be used in digital form.

While the embodiments of the present invention have been illustrated in detail, it should be apparent that modifications and adaptations to these embodiments may occur to one skilled in the art without departing from the scope of the present invention as set forth in the following claims. 

1-6. (canceled)
 7. A method of sensing the color of incident light comprising: capturing a portion of the incident light with a first semiconductor photodiode of a first material comprising silicon with a sensitivity peak at a first wavelength and generating a first photocurrent; capturing a portion of the incident light with a second semiconductor photodiode of a second material comprising silicon-germanium with a sensitivity peak at a second wavelength and generating a second photocurrent; and computing the ratio of the first photocurrent to the second photocurrent.
 8. The method of claim 7, where the step of computing the ratio of the first photocurrent to the second photocurrent further comprises: converting the first photocurrent to a first voltage representative of the first photocurrent, converting the second photocurrent to a second voltage representative of the second photocurrent, and computing the ratio of the first and second voltages.
 9. The method of claim 7, where the ratio is computed in analog form.
 10. The method of claim 8, where the ratio is computed in analog form.
 11. The method of claim 7, where the step of computing the ratio of the first photocurrent to the second photocurrent further comprises; converting the first photocurrent to a first digital representation of the first photocurrent, converting the second photocurrent to a second digital representation of the second photocurrent, and computing the ratio of the first and second digital representations. 